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What is the probability that an electron in the ground state of hydrogen will be found inside the nucleus?

  1. First calculate the exact answer, assuming the wave function is correct all the way down tor=0. Let b be the radius of the nucleus.
  2. Expand your result as a power series in the small numbera=2bla, and show that the lowest-order term is the cubic:P≈(4l3)(bla)3. This should be a suitable approximation, provided thatb≪a(which it is).
  3. Alternatively, we might assume thatψ(r)is essentially constant over the (tiny) volume of the nucleus, so thatP≈(4l3)πb3lψ(0)l2.Check that you get the same answer this way.
  4. Useb≈10-15manda≈0≈5×10-10mto get a numerical estimate forP. Roughly speaking, this represents the fraction of its time that the electron spends inside the nucleus:"

Short Answer

Expert verified

(a) Radius of the nucleus isP=1-1+2ba+2b2a2e-2bla

(b) Exponential up to the third power isP=43ba3

(c) Volume of the nucleus isP=43ba3.

(d) Numerical estimate forpisP=1.07×10-14.

Step by step solution

01

 Define the wave function

Hydrogen atoms ground state is described byψ100(r,θ,Ï•)=1Ï€²¹3e-r/a

02

 Find the probability

(a)

The probability of finding the electron inside a nucleus with radius is:

P=∫ψ2d3r=1πa3∫02π∫0π∫0be-2rlar2sinθdrdθdϕ=4ππa3∫0be-2rlar2dr=4a3-a2r2e-2rla+a34e-2rla-2ra-10b=-1+2ra+2r2a2e-2rla0b=1-1+2ba+22b2a2e-2rlaP=1-1+2ba+22b2a2e-2rla

Thus,

the probability is1-1+2ba+22b2a2e-2rla.

03

Expand the exponential up to the third power

(b)

Assume ε=2b/ain the result of part (a), and get,

P=1-1+∈+12∈2e-∈P=1-1+∈+12∈21-∈∈22-∈33!P=1-1+∈+12∈21-∈∈22-∈33!=1-1+∈-∈22+∈76-∈+∈2-∈22-∈22+∈22=∈316-12+11P=43ba3

Thus, the lowest order term is cubic.

04

Explain the essentially constant over the volume of the nucleus

(c)

Alternatively, let the wave function is constant across the nucleus' volume.

a≈0.5×10-10m=43πb3πa3=43ba3P=43ba3

Therefore, the result matches with the result of part b.

05

Find fraction of its time that the electron spends inside the nucleus

(d)

Calculate the probability by usingb≈10-15anda≈0.5×10-10

P=4310-150.5×10-103=432×10-53=43.8×10-15=323×10-15P1.07×10-14

Hence, the estimate for P is1.07×10-14.

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Most popular questions from this chapter

[Attempt this problem only if you are familiar with vector calculus.] Define the (three-dimensional) probability current by generalization of Problem 1.14:

J=ih2m(ψ∇ψ*-ψ*∇ψ)

(a) Show that satisfies the continuity equation ∇.J=-∂∂t|ψ|2which expresses local conservation of probability. It follows (from the divergence theorem) that ∫sJ.da=-ddt∫v|ψ|2d3rwhere Vis a (fixed) volume and is its boundary surface. In words: The flow of probability out through the surface is equal to the decrease in probability of finding the particle in the volume.

(b) FindJfor hydrogen in the staten=2,l=1,m=1 . Answer:

h64ma5re-r/a²õ¾±²Ôθϕ^

(c) If we interpretmJas the flow of mass, the angular momentum is

L=m∫(r×J)d3r

Use this to calculate Lzfor the stateψ211, and comment on the result.

Determine the commutator of S2withSZ(1)(whereS≡S(1)+S(2)) Generalize your result to show that

[S2,S1]=2Ih(S1×S2)

Comment: Because Sz(1)does not commute with S2, we cannot hope to find states that are simultaneous eigenvectors of both. In order to form eigenstates ofS2weneed linear combinations of eigenstates ofSz(1). This is precisely what the Clebsch-Gordan coefficients (in Equation 4.185) do for us, On the other hand, it follows by obvious inference from Equation 4.187that the sumrole="math" localid="1655980965321" S(1)+S(2)does commute withdata-custom-editor="chemistry" S2, which is a special case of something we already knew (see Equation 4.103).

An electron is at rest in an oscillating magnetic field

B=B0cos(Ó¬³Ù)k^

whereB0 andÓ¬ are constants.

(a) Construct the Hamiltonian matrix for this system.

(b) The electron starts out (at t=0 ) in the spin-up state with respect to the x-axis (that is:χ(0)=χ+(x)). Determine X(t)at any subsequent time. Beware: This is a time-dependent Hamiltonian, so you cannot get in the usual way from stationary states. Fortunately, in this case you can solve the timedependent Schrödinger equation (Equation 4.162) directly.

(c) Find the probability of getting-h/2 , if you measure Sx. Answer:

sin2(γµþ02Ó¬sin(Ó¬³Ù))

(d) What is the minimum field(B0) required to force a complete flip inSx ?

(a) Find〈r〉and〈r²〉for an electron in the ground state of hydrogen. Express your answers in terms of the Bohr radius.

(b) Find〈x〉and (x2)for an electron in the ground state of hydrogen.

Hint: This requires no new integration—note that r2=x2+y2+z2,and exploit the symmetry of the ground state.

(c) Find〈x²〉in the state n=2,l=1,m=1. Hint: this state is not symmetrical in x, y, z. Usex=rsinθcosπx=rsinθcosϕ

Work out the radial wave functions R30,R31,andR32using the recursion formula. Don’t bother to normalize them.

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